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1 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Gases Chapter 5 Become familiar with the definition and measurement of gas pressure. Learn the gas law and ideal gas equation. Understand the concept of the partial pressures. Study the kinetic molecular theory and gas Effusion/Diffusion Main differences between ideal and real gases. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

2 Elements that exist as gases at 250C and 1 atmosphere
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3 Physical Characteristics of Gases
Gases assume the volume and shape of their containers. Gases are the most compressible state of matter. Gases will mix evenly and completely when confined to the same container. Gases have much lower densities than liquids and solids. Exerts pressure on its surroundings. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

4 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Figure 5.1a: The pressure exerted by the gases in the atmosphere can be demonstrated by boiling water in a large metal can (a) and then turning off the heat and sealing the can. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

5 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Figure 5.01b: As the can cools, the water vapor condenses, lowering the gas pressure inside the can. This causes the can to crumple. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

6 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Force Area Pressure = Units of Pressure 1 pascal (Pa) = 1 N/m2 1 atm = 760 mmHg = 760 torr 1 atm = 101,325 Pa Copyright©2000 by Houghton Mifflin Company. All rights reserved.

7 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
10 miles 0.2 atm 4 miles 0.5 atm Sea level 1 atm Copyright©2000 by Houghton Mifflin Company. All rights reserved.

8 Copyright©2000 by Houghton Mifflin Company. All rights reserved.

9 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Boyle’s Law Copyright©2000 by Houghton Mifflin Company. All rights reserved.

10 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
As P (h) increases V decreases Copyright©2000 by Houghton Mifflin Company. All rights reserved.

11 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Boyle’s Law P a 1/V Constant temperature Constant amount of gas P x V = constant P1 x V1 = P2 x V2 Copyright©2000 by Houghton Mifflin Company. All rights reserved.

12 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Boyle’s Law* Pressure  Volume = Constant (T = constant) P1V1 = P2V2 (T = constant) V  1/P (T = constant) (*Holds precisely only at very low pressures.) Copyright©2000 by Houghton Mifflin Company. All rights reserved.

13 As pressure increases, the volume of SO2 decrease
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14 Copyright©2000 by Houghton Mifflin Company. All rights reserved.

15 A gas that strictly obeys Boyle’s Law is called an ideal gas.
Copyright©2000 by Houghton Mifflin Company. All rights reserved.

16 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
A sample of chlorine gas occupies a volume of 946 mL at a pressure of 726 mmHg. What is the pressure of the gas (in mmHg) if the volume is reduced at constant temperature to 154 mL? P1 x V1 = P2 x V2 P1 = 726 mmHg P2 = ? V1 = 946 mL V2 = 154 mL P1 x V1 V2 726 mmHg x 946 mL 154 mL = P2 = = 4460 mmHg Copyright©2000 by Houghton Mifflin Company. All rights reserved.

17 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Volume-Temperature Relationship As T increases V increases Copyright©2000 by Houghton Mifflin Company. All rights reserved.

18 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Charles's Law Figure 5.9: Plots of V versus T as in Fig. 5.8 except here the Kelvin scale is used for temperature. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

19 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Charles’s Law The volume of a gas is directly proportional to temperature, and extrapolates to zero at zero Kelvin. V = bT (P = constant) b = a proportionality constant Copyright©2000 by Houghton Mifflin Company. All rights reserved.

20 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Charles’s Law Copyright©2000 by Houghton Mifflin Company. All rights reserved.

21 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
A sample of carbon monoxide gas occupies 3.20 L at 125 0C. At what temperature will the gas occupy a volume of 1.54 L if the pressure remains constant? V1/T1 = V2/T2 V1 = 3.20 L V2 = 1.54 L T1 = K T2 = ? V2 x T1 V1 1.54 L x K 3.20 L = T2 = = 192 K Copyright©2000 by Houghton Mifflin Company. All rights reserved.

22 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Avogadro’s Law V a number of moles (n) Constant temperature Constant pressure V = constant x n V1/n1 = V2/n2 Copyright©2000 by Houghton Mifflin Company. All rights reserved.

23 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Figure 5.18: The effects of increasing the number of moles of gas particles at constant temperature and pressure. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

24 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Ideal Gas Equation Boyle’s law: V a (at constant n and T) 1 P Charles’ law: V a T (at constant n and P) Avogadro’s law: V a n (at constant P and T) V a nT P V = constant x = R nT P R is the gas constant PV = nRT Copyright©2000 by Houghton Mifflin Company. All rights reserved.

25 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Ideal Gas Law PV = nRT R = proportionality constant = L atm  mol P = pressure in atm V = volume in liters n = moles T = temperature in Kelvins Holds closely at P < 1 atm Copyright©2000 by Houghton Mifflin Company. All rights reserved.

26 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
The conditions 0 0C and 1 atm are called standard temperature and pressure (STP). Experiments show that at STP, 1 mole of an ideal gas occupies L. PV = nRT R = PV nT = (1 atm)(22.42L) (1 mol)( K) R = L • atm / (mol • K) Copyright©2000 by Houghton Mifflin Company. All rights reserved.

27 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
What is the volume (in liters) occupied by 49.8 g of HCl at STP? T = 0 0C = K P = 1 atm PV = nRT n = 49.8 g x 1 mol HCl 36.45 g HCl = 1.37 mol V = nRT P V = 1 atm 1.37 mol x x K L•atm mol•K V = 30.6 L Copyright©2000 by Houghton Mifflin Company. All rights reserved.

28 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Argon is an inert gas used in lightbulbs to retard the vaporization of the filament. A certain lightbulb containing argon at 1.20 atm and 18 0C is heated to 85 0C at constant volume. What is the final pressure of argon in the lightbulb (in atm)? PV = nRT n, V and R are constant nR V = P T = constant P1 = 1.20 atm T1 = 291 K P2 = ? T2 = 358 K P1 T1 P2 T2 = P2 = P1 x T2 T1 = 1.20 atm x 358 K 291 K = 1.48 atm Copyright©2000 by Houghton Mifflin Company. All rights reserved.

29 Density (d) Calculations
m is the mass of the gas in g m V = PM RT d = M is the molar mass of the gas Molar Mass (M ) of a Gaseous Substance dRT P M = d is the density of the gas in g/L Copyright©2000 by Houghton Mifflin Company. All rights reserved.

30 Gas Stoichiometry What is the volume of CO2 produced at 370 C and 1.00 atm when 5.60 g of glucose are used up in the reaction: C6H12O6 (s) + 6O2 (g) CO2 (g) + 6H2O (l) g C6H12O mol C6H12O mol CO V CO2 1 mol C6H12O6 180 g C6H12O6 x 6 mol CO2 1 mol C6H12O6 x 5.60 g C6H12O6 = mol CO2 0.187 mol x x K L•atm mol•K 1.00 atm = nRT P V = = 4.76 L Copyright©2000 by Houghton Mifflin Company. All rights reserved. 5.5

31 Dalton’s Law of Partial Pressures
For a mixture of gases in a container, PTotal = P1 + P2 + P Copyright©2000 by Houghton Mifflin Company. All rights reserved.

32 Dalton’s Law of Partial Pressures
V and T are constant P1 P2 Ptotal = P1 + P2 Copyright©2000 by Houghton Mifflin Company. All rights reserved.

33 PA = nART V PB = nBRT V XA = nA nA + nB XB = nB nA + nB PT = PA + PB
Consider a case in which two gases, A and B, are in a container of volume V. PA = nART V nA is the number of moles of A PB = nBRT V nB is the number of moles of B XA = nA nA + nB XB = nB nA + nB PT = PA + PB PA = XA PT PB = XB PT Pi = Xi PT Copyright©2000 by Houghton Mifflin Company. All rights reserved.

34 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
A sample of natural gas contains 8.24 moles of CH4, moles of C2H6, and moles of C3H8. If the total pressure of the gases is 1.37 atm, what is the partial pressure of propane (C3H8)? Pi = Xi PT PT = 1.37 atm 0.116 Xpropane = = Ppropane = x 1.37 atm = atm Copyright©2000 by Houghton Mifflin Company. All rights reserved.

35 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Water Vapor Pressure Copyright©2000 by Houghton Mifflin Company. All rights reserved.

36 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Bottle full of oxygen gas and water vapor 2KClO3 (s) KCl (s) + 3O2 (g) PT = PO + PH O 2 Copyright©2000 by Houghton Mifflin Company. All rights reserved.

37 Kinetic Molecular Theory of Gases
A gas is composed of molecules that are separated from each other by distances far greater than their own dimensions. The molecules can be considered to be points that is, they possess mass but have negligible volume (V  zero). Gas molecules are in constant motion in random directions. Collisions among molecules are perfectly elastic. Gas molecules exert neither attractive nor repulsive forces on one another. The average kinetic energy of the molecules is proportional to the temperature of the gas in kelvins. Any two gases at the same temperature will have the same average kinetic energy Copyright©2000 by Houghton Mifflin Company. All rights reserved.

38 Kinetic theory of gases and …
Compressibility of Gases Boyle’s Law P a collision rate with wall Collision rate a number density Number density a 1/V P a 1/V Charles’ Law Collision rate a average kinetic energy of gas molecules Average kinetic energy a T P a T Copyright©2000 by Houghton Mifflin Company. All rights reserved.

39 Kinetic theory of gases and …
Avogadro’s Law P a collision rate with wall Collision rate a number density Number density a n P a n Dalton’s Law of Partial Pressures Molecules do not attract or repel one another P exerted by one type of molecule is unaffected by the presence of another gas Ptotal = SPi Copyright©2000 by Houghton Mifflin Company. All rights reserved.

40 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Figure 5.19: Path of one particle in a gas. Any given particle will continuously change its course as a result of collisions with other particles, as well as with the walls of the container: The concept of Average Speed Copyright©2000 by Houghton Mifflin Company. All rights reserved.

41  3RT urms = M The distribution of speeds of three different gases
at the same temperature The distribution of speeds for nitrogen gas molecules at three different temperatures urms = 3RT M Note: M in Kg per mole Copyright©2000 by Houghton Mifflin Company. All rights reserved.

42 The Meaning of Temperature
Kelvin temperature is an index of the random motions of gas particles (higher T means greater motion.) Copyright©2000 by Houghton Mifflin Company. All rights reserved.

43 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Diffusion: describes the mixing of gases. The rate of diffusion is the rate of gas mixing. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

44 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Gas diffusion is the gradual mixing of molecules of one gas with molecules of another by virtue of their kinetic properties. NH4Cl NH3 17 g/mol HCl 36 g/mol Copyright©2000 by Houghton Mifflin Company. All rights reserved.

45 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Effusion: describes the passage of gas into an evacuated chamber. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

46 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Effusion: Diffusion: Copyright©2000 by Houghton Mifflin Company. All rights reserved.

47 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Real Gases Must correct ideal gas behavior when at high pressure (smaller volume) and low temperature (attractive forces become important). Copyright©2000 by Houghton Mifflin Company. All rights reserved.

48 Figure 5.25: Plots of PV/nRT versus P for several gases (200 K).
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49 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Figure 5.26: Plots of PV/nRT versus P for nitrogen gas at three temperatures. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

50 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Figure 5.27: (a) Gas at low concentration— relatively few interactions between particles. (b) Gas at high concentration—many more interactions between particles. Copyright©2000 by Houghton Mifflin Company. All rights reserved.

51 Copyright©2000 by Houghton Mifflin Company. All rights reserved.
Real Gases corrected pressure corrected volume Pideal Videal Copyright©2000 by Houghton Mifflin Company. All rights reserved.

52 Copyright©2000 by Houghton Mifflin Company. All rights reserved.


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